. .. Introduction, 119 5.2.1 Motivation: generation of low-energy high order plasmon modes

. .. Dimer-coupling-of-nanocrosses, 124 5.2.4.1 Hybridization model for localized surface plasmon

. .. , Summary of the different spectral tuning processes, p.127

. , Self-hybridization within non-Hermitian localized plasmonic systems

. , 128 5.3.1.2 The growing field of non-Hermitian physics, p.128

. .. Eigenproblem, 3.2.3 Symmetry analysis of the overlap matrix, p.133

. , LSP vs. electromagnetic wave in open systems

. .. Resonator, 135 5.3.4.1 Mode mixing within the BEM perturbation theory

. .. , 138 5.3.6 Physical origin of plasmonic bi-orthogonality

. .. , History of the local continuum dielectric model, p.160

. .. Phonons, 163 6.4.3 Analogy between localized SP and cSPh modes

E. .. , 164 6.5.2 Comparison with optical experiments, p.165

, General properties of confined surface phonon modes, p.166

. , Fuchs-Kliewer modes of thin material slabs

.. .. Substrate,

P. .. Summary,

, ? Hydrodynamical models which naturally take non-linearities into account, vol.447

, Matloob used the Langevin equations to quantize the EM field in absorbing media and dieletrics. The Lindblad equation, which is basically the quantum form of the Markovian master equation, is a standard technique in optomechanics and atomic physics, ? Nonequilibrium statistical methods such as quantum Langevin equations or Lindblad equation for the density matrix

, These methods are heavier in terms of computation but also give more general and versatile expressions, ? Propagator formalism and diagrammatic expansions

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